Research/Sitter/MAGNDATA / 0.804_MoP3SiO11.mcif
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| Magnetic group | C 2/c′ BNS 15.88 |
| Point group | 2/m′ |
| Parent space group | R 3 c No. 167 |
| Spins | collinear · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 8.4015 · b 8.4015 · c 39.8466 Å · α 90° · β 90° · γ 120° |
| Transition | 6.8 K (−266 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Mo |
| Largest moment component | 3.0415 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Mo | Mo | 0 | 0 | 0.1593 | 1.5208 | 3.0415 | 0 | 2.634 |
| P_1 | P | 0.3702 | 0.0323 | 0.119 | ||||
| P_2 | P | 0.9677 | 0.3379 | 0.119 | ||||
| P_3 | P | 0.6621 | 0.6298 | 0.119 | ||||
| Si | Si | 0 | 0 | 0.4607 | ||||
| O1_1 | O | 0.2879 | 0.818 | 0.1134 | ||||
| O1_2 | O | 0.182 | 0.4699 | 0.1134 | ||||
| O1_3 | O | 0.5301 | 0.7121 | 0.1134 | ||||
| O2_1 | O | 0.2237 | 0.075 | 0.1271 | ||||
| O2_2 | O | 0.925 | 0.1487 | 0.1271 | ||||
| O2_3 | O | 0.8513 | 0.7763 | 0.1271 | ||||
| O3_1 | O | 0.5282 | 0.1048 | 0.1434 | ||||
| O3_2 | O | 0.8952 | 0.4234 | 0.1434 | ||||
| O3_3 | O | 0.5766 | 0.4718 | 0.1434 | ||||
| O4_1 | O | 0.4524 | 0 | 0.25 | ||||
| O4_2 | O | 0 | 0.4524 | 0.25 | ||||
| O5 | O | 0 | 0 | 0 |
Moment components are along the crystal axes a, b, c (μB), as magCIF writes them. Symmetry generates the rest of the cell from these sites.
D. I. Badrtdinov et al. PHYSICAL REVIEW B (2021) · doi:10.1103/PhysRevB.104.094428
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.804_MoP3SiO11.mcif from MAGNDATA · entry page
sha256 of this copy: 60d02aec1fa20bd2d9c4b8122c4aa0cdd80ef0a0f9d8da96bd6467432be493ab
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.804_MoP3SiO11.mcif.